Please use this identifier to cite or link to this item: http://hdl.handle.net/20.500.12323/4660
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dc.contributor.authorGunes, Hikmet-
dc.contributor.authorKerimov, Nazim B.-
dc.contributor.authorKaya, Ufuk-
dc.date.accessioned2020-08-09T07:30:46Z-
dc.date.available2020-08-09T07:30:46Z-
dc.date.issued2015-
dc.identifier.citationResults in Mathematicsen_US
dc.identifier.urihttp://hdl.handle.net/20.500.12323/4660-
dc.description.abstractIn this paper, we consider the following periodic and antiperiodic problem yiv + p2 (x) y + p1 (x) y + p0 (x) y = λy, 0 <x< 1, y(s) (1) − (−1)σ y(s) (0) = 0, s = 0, 3, where λ is a spectral parameter; pj (x) ∈ L1(0, 1), j = 0, 1, p2(x) ∈ W1 1 (0, 1) with 1 0 p2(ξ)dξ = 0 are complex-valued functions and σ = 0, 1. The boundary conditions of this problem are periodic-antiperiodic boundary conditions and it is well known that they are regular but not strongly regular. Asymptotic formulae for eigenvalues and eigenfunctions of the considered boundary value problem are established. Under the condition (p2 (1) − p2 (0) − 2c1) (p2 (1) − p2 (0) + 2c1) = 0, it is proved that all the eigenvalues (except for finite number) are simple, where c1 = 1 0 p1(ξ)dξ. Furthermore, we prove that the system of root functions of this spectral problem forms a basis in the space Lp(0, 1), 1 <p< ∞, when p1(1) = p1(0); p(s) 2 (1) = p(s) 2 (0), s = 0, 1; pj (x) ∈ Wj 1 (0, 1), j = 0, 1, 2; c1 = 0. Also, it is shown that this basis is unconditional for p = 2.en_US
dc.language.isoenen_US
dc.publisherSpringer Baselen_US
dc.relation.ispartofseriesVol. 68;№ 3-4-
dc.subjectFourth order eigenvalue problemen_US
dc.subjectperiodic and antiperiodic boundary conditionsen_US
dc.subjectasymptotic behavior of eigenvalues and eigenfunctionsen_US
dc.subjectbasis properties of the system of root functionsen_US
dc.titleSpectral Properties of Fourth Order Differential Operators with Periodic and Antiperiodic Boundary Conditionsen_US
dc.typeArticleen_US
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